低压电弧槽电弧劈裂过程建模

A. Mutzke, T. Ruther, M. Kurrat, M. Lindmayer, Ernst-Dieter Wilkening
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引用次数: 28

摘要

对低压电弧槽中电弧分裂过程的研究表明,在新的电弧根形成之前,必须超过一个阈值电压。当形成电弧点时,电极下降几乎是恒定的,与电流无关。在模拟中,在分流板周围有一层具有非线性电流密度-电压特性的薄层元件代表了新电弧根的形成。为了模拟这种行为,在以前的出版物中提出了低电流密度下电压驼峰和高电流密度下恒定的最终电压的特征。本文研究了电压驼峰幅度的影响。电压较低的驼峰产生一个更小的电弧环,围绕分裂板的前缘和更早的电弧细分。电压过高的驼峰使电弧不可能分裂。通过不使用弧根模型而只考虑金属板的特性的对比仿真,可以看出,要真实地模拟弧裂过程,需要对弧根进行特殊处理。并在实验结果的基础上进行了比较和验证。在此基础上,分析了电弧劈裂过程中通过极板的电弧电压、电弧电流以及电弧根的位置。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Modeling the Arc Splitting Process in Low-Voltage Arc Chutes
Investigations on the arc splitting process in low- voltage arc chutes have shown that a threshold voltage has to be exceeded before new arc roots form. When an arc spot has been formed, the electrode fall is nearly constant and rather independent of the current. In simulations a thin layer of elements with a nonlinear current density-voltage characteristic surrounding the splitter plate represents the formation of new arc roots. To model this behavior a characteristic with a voltage hump at low current densities and a constant final voltage at higher current densities has been presented in former publications. In this paper, the influence of the magnitude of the voltage hump is studied. A lower voltage hump yields a smaller arc loop around the front edge of the splitter plate and an earlier subdivision of the arc. A too high voltage hump makes arc splitting impossible. A comparing simulation without any arc root model, but only with the properties of the metallic plates, shows that a realistic simulation of the arc splitting process needs special treatment of the arc roots. The results are compared and verified on the basis of experimental results. Hence, the arc splitting process is analyzed concerning arc voltage and current through the plate as well as location of the arc roots.
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